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image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Proceedings of the I...arrow_drop_down
image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao
Proceedings of the IEEE
Article . 1973 . Peer-reviewed
License: IEEE Copyright
Data sources: Crossref
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Magnetic shielding for magnetically levitated vehicles

Authors: Y. Iwasa;

Magnetic shielding for magnetically levitated vehicles

Abstract

The magnetic shielding required for magnetically levitated vehicles is discussed. Shielding is needed to protect passengers in a vehicle from stray dc magnetic fields coming from the superconducting dipoles carried by the vehicle. In addition, the superconducting dipoles must be shielded against various ac magnetic fields. Here we consider shielding of ac magnetic fields generated by the propulsion windings for the case of a linear-synchronous-motor active guideway. Protection for passengers against magnetic fields is necessary as there are at present no data upon which to base a human tolerance of magnetic-field intensity. It is shown here that in a magnetically levitated vehicle where the space to be shielded is large and where the weight of shielding is a prime concern, active shielding, in which compensation dipoles generate a canceling magnetic field, is superior to passive shielding, which uses iron plates. At the floor of the passenger cabin of a proposed vehicle, the magnetic field, without compensation, is as high as 0.03 T. Compensation dipoles, comparable in size to and placed 0.5 m above the main dipoles, increase the total conductor requirement by about ⅓ to bring the magnetic field at the floor of the passenger cabin below a level of 0.005 T. To achieve the same result by passive shielding, an iron plate or equivalent up to 2 cm thick must cover the floor of the passenger cabin, resulting in at least a 10 000-kg increase in the total weight for a 100-passenger vehicle. We therefore strongly recommend active shielding. At 100 Hz, a peak ac field of more than 10-5T cannot be tolerated in the superconducting dipoles of a vehicle as hysteresis and eddy-current losses within the conductor become excessive. The ac field reaching the main dipoles from the propulsion windings in the guideway can be as high as 10-3T without shielding. An aluminum sheet of 2-mm thickness kept at 4.2 K attenuates the field and makes ac superconductor losses negligible while keeping the eddy-current losses in the sheet to an acceptable level.

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selected citations
These citations are derived from selected sources.
This is an alternative to the "Influence" indicator, which also reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Citations provided by BIP!
popularity
This indicator reflects the "current" impact/attention (the "hype") of an article in the research community at large, based on the underlying citation network.
BIP!Popularity provided by BIP!
influence
This indicator reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Influence provided by BIP!
impulse
This indicator reflects the initial momentum of an article directly after its publication, based on the underlying citation network.
BIP!Impulse provided by BIP!
14
Average
Top 10%
Top 10%
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